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In the title hydrate, [Pt(CH3)3(CH3COO)(C10H8N2)]·H2O, the PtIV atom exhibits a distorted octa­hedral coordination geometry built up by three methyl ligands in a facial arrangement, a bipyridine ligand and a monodentately bound acetate ligand. In the crystal structure, inter­molecular O—H...O hydrogen bonds are observed between the water mol­ecule and the platinum complex, which link the mol­ecules into chains along the c axis.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053681000499X/tk2621sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053681000499X/tk2621Isup2.hkl
Contains datablock I

CCDC reference: 769874

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.019 Å
  • R factor = 0.040
  • wR factor = 0.119
  • Data-to-parameter ratio = 14.7

checkCIF/PLATON results

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Alert level C PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for Pt1 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C4 PLAT245_ALERT_2_C U(iso) H21 Smaller than U(eq) O3 by ... 0.02 AngSq PLAT342_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang .. 19 PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.595 2 PLAT971_ALERT_2_C Large Calcd. Non-Metal Positive Residual Density 1.55 eA-3 PLAT153_ALERT_1_C The su's on the Cell Axes are Equal (x 100000) 300 Ang. PLAT234_ALERT_4_C Large Hirshfeld Difference N1 -- C10 .. 0.15 Ang.
Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 2 PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature 293 K PLAT380_ALERT_4_G Check Incorrectly? Oriented X(sp2)-Methyl Moiety C5
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 8 ALERT level C = Check and explain 4 ALERT level G = General alerts; check 3 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 4 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Due to the low-spin d6 electron configuration of platinum(IV), ligand substitution reactions of their complexes may be hampered. Starting from complexes having a PtMe3 unit (Vetter et al., 2006; Clegg et al., 1972; Lindner et al., 2008), substitution reactions were found to proceed smoothly even with weak donors (Steinborn & Junicke, 2000) because the leaving ligand is additionally activated by the high trans effect exerted by the methyl ligand.

The asymmetric unit of the title hydrate comprises a neutral platinum complex, [PtMe3(OAc-κO)(bpy)], and a water molecule. The primary coordination sphere of the platinum atom is built up by three methyl ligands in facial binding fashion, a bipyridine ligand and a monodentately bound acetato ligand. As expected for Pt(IV) complexes, an octahedral coordination geometry was found, which is distorted due to the restricted bite of the 2,2'-bipyridine ligand [N1—Pt1—N2 76.7 (3)°]; the other angles between cis arranged ligands are between 85.1 (5) and 99.9 (4)°. Due to the high trans influence of the methyl ligands the Pt1—O1 bond was found to be relatively long (2.168 (6) Å) compared to those of other carboxylato platinum(IV) [median: 2.013, lower/upper quartile: 2.001/2.044 Å, 496 observations taken from the CSD, version 5.30 (Allen, 2002)]. In the crystal structure quite strong intermolecular O—H···O hydrogen bonds were found in which the water molecules act as hydrogen donors and the oxygen atoms of acetato ligand as hydrogen acceptors (Table 1). Due to these hydrogen bonds the molecules are linked in infinite chains along the c axis.

Related literature top

For ligand-substitution reactions of platinum complexes, see: Vetter et al. (2006); Clegg et al.(1972); Lindner et al. (2008); Steinborn & Junicke (2000). For a description of the Cambridge Structural Database, see: Allen (2002).

Experimental top

Under anaerobic conditions [(PtMe3I)4] (50 mg, 0.03 mmol) and AgOAc (23 mg, 0.14 mmol) were stirred in acetone (10 ml) for 15 h in the absence of light. The precipitated AgI was filtered off and the solvent was reduced in vacuo to 3 ml. Then n-pentane was added and the white precipitate was collected by filtration, washed with n-pentane (2 × 1 ml) and recrystallized from chloroform.

Refinement top

The water-H atoms were found in a difference map and refined with each O—H distance restrained to 0.85 (1) Å. All other H atoms were positioned geometrically and allowed to ride on the respective parent atoms with C—H = 0.93–0.96 Å [Uiso(H) = 1.2 Ueq(C)]. The maximum and minimum residual electron density peaks of 1.61 and -1.79 e Å-3, respectively, were located 1.19 Å and 1.21 Å from the Pt1 atom.

Computing details top

Data collection: STADI4 (Stoe & Cie, 1996); cell refinement: STADI4 (Stoe & Cie, 1996); data reduction: STADI4 (Stoe & Cie, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2001); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Structure of the asymmetric unit of the title hydrate [PtMe3(OAc-κO)(bpy)].H2O. Displacement ellipsoids are drawn at the 30% probability level and the H atoms are shown as small spheres of arbitrary radii.
(Acetato-κO)(2,2'-bipyridine-κ2N,N')trimethylplatinum(IV) monohydrate top
Crystal data top
[Pt(CH3)3(C2H3O2)(C10H8N2)]·H2OF(000) = 912
Mr = 473.44Dx = 1.890 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 26 reflections
a = 10.972 (3) Åθ = 15.1–25.2°
b = 13.455 (3) ŵ = 8.44 mm1
c = 13.768 (3) ÅT = 293 K
β = 125.05 (3)°Block, orange
V = 1663.9 (8) Å30.48 × 0.34 × 0.24 mm
Z = 4
Data collection top
Stoe STADI-IV
diffractometer
2455 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.031
Graphite monochromatorθmax = 25.0°, θmin = 2.3°
ω/2θ scansh = 1313
Absorption correction: ψ scan
(X-RED32; Stoe & Cie, 1996)
k = 160
Tmin = 0.031, Tmax = 0.089l = 1316
4494 measured reflections2 standard reflections every 60 min
2931 independent reflections intensity decay: random, +5%
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.119 w = 1/[σ2(Fo2) + (0.0676P)2 + 4.3682P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
2931 reflectionsΔρmax = 1.61 e Å3
199 parametersΔρmin = 1.79 e Å3
2 restraintsExtinction correction: SHELXL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 constraintsExtinction coefficient: 0.0018 (3)
Primary atom site location: structure-invariant direct methods
Crystal data top
[Pt(CH3)3(C2H3O2)(C10H8N2)]·H2OV = 1663.9 (8) Å3
Mr = 473.44Z = 4
Monoclinic, P21/cMo Kα radiation
a = 10.972 (3) ŵ = 8.44 mm1
b = 13.455 (3) ÅT = 293 K
c = 13.768 (3) Å0.48 × 0.34 × 0.24 mm
β = 125.05 (3)°
Data collection top
Stoe STADI-IV
diffractometer
2455 reflections with I > 2σ(I)
Absorption correction: ψ scan
(X-RED32; Stoe & Cie, 1996)
Rint = 0.031
Tmin = 0.031, Tmax = 0.0892 standard reflections every 60 min
4494 measured reflections intensity decay: random, +5%
2931 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0402 restraints
wR(F2) = 0.119H atoms treated by a mixture of independent and constrained refinement
S = 1.06Δρmax = 1.61 e Å3
2931 reflectionsΔρmin = 1.79 e Å3
199 parameters
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.0620 (12)0.7592 (8)0.1850 (9)0.072 (3)
H10.05350.76730.11980.087*
H30.16290.77140.15840.087*
H20.03450.69260.21500.087*
C20.0048 (12)0.7967 (10)0.4045 (11)0.081 (3)
H60.04120.82840.48040.097*
H50.01700.72690.41580.097*
H40.11060.80630.35910.097*
C30.0935 (11)0.9574 (8)0.2409 (10)0.069 (3)
H90.06031.01750.28690.083*
H80.17600.93040.23870.083*
H70.12410.97180.16160.083*
C40.3091 (10)0.7018 (7)0.3608 (9)0.058 (2)
C50.4295 (13)0.6271 (9)0.4412 (12)0.081 (4)
H110.46360.59500.39860.098*
H100.38990.57820.46670.098*
H120.51130.66080.50910.098*
C60.2491 (12)0.9787 (10)0.5540 (9)0.077 (3)
H130.20510.93580.57840.093*
C70.3426 (14)1.0548 (11)0.6304 (10)0.092 (4)
H140.35831.06380.70380.110*
C80.4096 (15)1.1153 (11)0.5953 (15)0.098 (5)
H150.47381.16520.64540.117*
C90.3823 (12)1.1025 (9)0.4859 (13)0.085 (4)
H160.42761.14370.46110.102*
C100.2869 (9)1.0279 (7)0.4123 (9)0.058 (2)
C110.2542 (10)1.0116 (7)0.2937 (9)0.057 (2)
C120.3080 (12)1.0709 (9)0.2434 (14)0.085 (4)
H170.36481.12710.28290.102*
C130.2752 (16)1.0446 (13)0.1327 (15)0.098 (5)
H180.31031.08320.09750.117*
C140.1935 (17)0.9642 (12)0.0776 (12)0.091 (4)
H190.17190.94590.00410.109*
C150.1410 (13)0.9078 (9)0.1301 (9)0.069 (3)
H200.08460.85140.09110.083*
N10.2221 (8)0.9665 (5)0.4471 (6)0.0486 (16)
N20.1687 (8)0.9318 (6)0.2344 (6)0.0525 (17)
O10.2551 (7)0.7497 (5)0.4062 (6)0.0615 (17)
O20.2727 (10)0.7105 (7)0.2563 (8)0.089 (2)
O30.4338 (10)0.7587 (8)0.6577 (9)0.088 (3)
H210.382 (12)0.767 (9)0.685 (10)0.07 (4)*
H220.379 (15)0.763 (12)0.580 (10)0.12 (6)*
Pt10.07572 (3)0.85719 (3)0.31606 (3)0.04758 (19)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.077 (7)0.052 (6)0.069 (7)0.020 (5)0.031 (6)0.003 (5)
C20.070 (6)0.095 (9)0.094 (8)0.007 (6)0.057 (6)0.031 (7)
C30.057 (5)0.067 (7)0.075 (7)0.015 (5)0.033 (5)0.015 (5)
C40.058 (5)0.050 (5)0.066 (6)0.001 (4)0.036 (5)0.008 (5)
C50.071 (7)0.076 (8)0.100 (9)0.017 (6)0.050 (7)0.004 (6)
C60.075 (7)0.102 (9)0.054 (6)0.018 (6)0.036 (5)0.005 (6)
C70.079 (8)0.108 (11)0.054 (6)0.023 (8)0.018 (6)0.027 (7)
C80.069 (8)0.082 (9)0.107 (12)0.003 (6)0.030 (8)0.035 (8)
C90.055 (6)0.068 (7)0.103 (10)0.002 (5)0.029 (6)0.020 (7)
C100.043 (4)0.049 (5)0.073 (6)0.009 (4)0.027 (4)0.003 (4)
C110.055 (5)0.055 (6)0.072 (6)0.018 (4)0.042 (5)0.017 (5)
C120.066 (6)0.070 (7)0.134 (12)0.007 (6)0.067 (7)0.031 (8)
C130.095 (9)0.120 (13)0.116 (12)0.016 (8)0.083 (9)0.047 (10)
C140.106 (9)0.121 (12)0.079 (8)0.039 (9)0.072 (8)0.037 (8)
C150.088 (7)0.078 (7)0.058 (6)0.014 (6)0.051 (6)0.003 (5)
N10.048 (4)0.051 (4)0.048 (4)0.009 (3)0.029 (3)0.006 (3)
N20.056 (4)0.058 (4)0.052 (4)0.008 (4)0.036 (3)0.009 (4)
O10.063 (4)0.062 (4)0.055 (4)0.014 (3)0.032 (3)0.006 (3)
O20.108 (6)0.095 (6)0.084 (6)0.025 (5)0.067 (5)0.014 (5)
O30.070 (5)0.118 (8)0.068 (5)0.001 (5)0.035 (5)0.014 (5)
Pt10.0491 (2)0.0487 (3)0.0473 (3)0.00074 (14)0.02902 (18)0.00514 (14)
Geometric parameters (Å, º) top
C1—Pt12.036 (10)C7—H140.9300
C1—H10.9600C8—C91.37 (2)
C1—H30.9600C8—H150.9300
C1—H20.9600C9—C101.382 (15)
C2—Pt12.041 (11)C9—H160.9300
C2—H60.9600C10—N11.345 (13)
C2—H50.9600C10—C111.474 (15)
C2—H40.9600C11—N21.349 (13)
C3—Pt12.032 (9)C11—C121.391 (15)
C3—H90.9600C12—C131.40 (2)
C3—H80.9600C12—H170.9300
C3—H70.9600C13—C141.33 (2)
C4—O21.258 (13)C13—H180.9300
C4—O11.259 (12)C14—C151.381 (17)
C4—C51.518 (14)C14—H190.9300
C5—H110.9600C15—N21.326 (12)
C5—H100.9600C15—H200.9300
C5—H120.9600N1—Pt12.161 (7)
C6—N11.335 (13)N2—Pt12.152 (7)
C6—C71.403 (18)O1—Pt12.168 (6)
C6—H130.9300O3—H210.85 (9)
C7—C81.36 (2)O3—H220.88 (11)
Pt1—C1—H1109.5N1—C10—C11117.4 (8)
Pt1—C1—H3109.5C9—C10—C11121.4 (11)
H1—C1—H3109.5N2—C11—C12120.2 (11)
Pt1—C1—H2109.5N2—C11—C10115.6 (8)
H1—C1—H2109.5C12—C11—C10124.2 (11)
H3—C1—H2109.5C11—C12—C13118.7 (13)
Pt1—C2—H6109.5C11—C12—H17120.6
Pt1—C2—H5109.5C13—C12—H17120.6
H6—C2—H5109.5C14—C13—C12119.7 (12)
Pt1—C2—H4109.5C14—C13—H18120.2
H6—C2—H4109.5C12—C13—H18120.2
H5—C2—H4109.5C13—C14—C15119.7 (13)
Pt1—C3—H9109.5C13—C14—H19120.1
Pt1—C3—H8109.5C15—C14—H19120.1
H9—C3—H8109.5N2—C15—C14121.9 (12)
Pt1—C3—H7109.5N2—C15—H20119.1
H9—C3—H7109.5C14—C15—H20119.1
H8—C3—H7109.5C6—N1—C10119.3 (9)
O2—C4—O1126.2 (9)C6—N1—Pt1126.3 (8)
O2—C4—C5117.9 (10)C10—N1—Pt1114.4 (6)
O1—C4—C5116.0 (10)C15—N2—C11119.8 (9)
C4—C5—H11109.5C15—N2—Pt1124.8 (8)
C4—C5—H10109.5C11—N2—Pt1115.4 (6)
H11—C5—H10109.5C4—O1—Pt1126.0 (6)
C4—C5—H12109.5H21—O3—H22112 (10)
H11—C5—H12109.5C3—Pt1—C189.0 (5)
H10—C5—H12109.5C3—Pt1—C289.2 (5)
N1—C6—C7121.4 (13)C1—Pt1—C285.1 (5)
N1—C6—H13119.3C3—Pt1—N289.6 (4)
C7—C6—H13119.3C1—Pt1—N299.9 (4)
C8—C7—C6118.8 (13)C2—Pt1—N2174.8 (5)
C8—C7—H14120.6C3—Pt1—N189.8 (4)
C6—C7—H14120.6C1—Pt1—N1176.5 (4)
C7—C8—C9119.7 (13)C2—Pt1—N198.2 (4)
C7—C8—H15120.1N2—Pt1—N176.7 (3)
C9—C8—H15120.1C3—Pt1—O1176.2 (4)
C8—C9—C10119.6 (14)C1—Pt1—O192.5 (4)
C8—C9—H16120.2C2—Pt1—O187.4 (4)
C10—C9—H16120.2N2—Pt1—O193.6 (3)
N1—C10—C9121.2 (11)N1—Pt1—O188.9 (3)
N1—C6—C7—C81.9 (18)C12—C11—N2—Pt1173.8 (7)
C6—C7—C8—C92 (2)C10—C11—N2—Pt17.6 (9)
C7—C8—C9—C100.1 (19)O2—C4—O1—Pt13.0 (15)
C8—C9—C10—N11.1 (16)C5—C4—O1—Pt1177.2 (7)
C8—C9—C10—C11179.9 (10)C15—N2—Pt1—C392.8 (8)
N1—C10—C11—N24.0 (12)C11—N2—Pt1—C383.5 (7)
C9—C10—C11—N2175.0 (9)C15—N2—Pt1—C13.8 (9)
N1—C10—C11—C12177.5 (9)C11—N2—Pt1—C1172.4 (6)
C9—C10—C11—C123.5 (14)C15—N2—Pt1—N1177.3 (8)
N2—C11—C12—C131.7 (15)C11—N2—Pt1—N16.4 (6)
C10—C11—C12—C13176.7 (10)C15—N2—Pt1—O189.3 (8)
C11—C12—C13—C140.2 (19)C11—N2—Pt1—O194.5 (6)
C12—C13—C14—C150 (2)C6—N1—Pt1—C393.0 (9)
C13—C14—C15—N20.5 (18)C10—N1—Pt1—C385.4 (7)
C7—C6—N1—C100.7 (15)C6—N1—Pt1—C23.8 (9)
C7—C6—N1—Pt1177.7 (8)C10—N1—Pt1—C2174.6 (6)
C9—C10—N1—C60.8 (13)C6—N1—Pt1—N2177.4 (8)
C11—C10—N1—C6179.8 (8)C10—N1—Pt1—N24.2 (6)
C9—C10—N1—Pt1179.3 (7)C6—N1—Pt1—O183.4 (8)
C11—C10—N1—Pt11.7 (10)C10—N1—Pt1—O198.2 (6)
C14—C15—N2—C112.0 (15)C4—O1—Pt1—C153.9 (8)
C14—C15—N2—Pt1174.0 (8)C4—O1—Pt1—C2138.9 (9)
C12—C11—N2—C152.6 (13)C4—O1—Pt1—N246.2 (8)
C10—C11—N2—C15176.0 (8)C4—O1—Pt1—N1122.8 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H22···O10.88 (11)1.96 (11)2.836 (12)172 (15)
O3—H21···O2i0.85 (9)1.96 (10)2.810 (14)177 (11)
Symmetry code: (i) x, y+3/2, z+1/2.

Experimental details

Crystal data
Chemical formula[Pt(CH3)3(C2H3O2)(C10H8N2)]·H2O
Mr473.44
Crystal system, space groupMonoclinic, P21/c
Temperature (K)293
a, b, c (Å)10.972 (3), 13.455 (3), 13.768 (3)
β (°) 125.05 (3)
V3)1663.9 (8)
Z4
Radiation typeMo Kα
µ (mm1)8.44
Crystal size (mm)0.48 × 0.34 × 0.24
Data collection
DiffractometerStoe STADI-IV
diffractometer
Absorption correctionψ scan
(X-RED32; Stoe & Cie, 1996)
Tmin, Tmax0.031, 0.089
No. of measured, independent and
observed [I > 2σ(I)] reflections
4494, 2931, 2455
Rint0.031
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.119, 1.06
No. of reflections2931
No. of parameters199
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)1.61, 1.79

Computer programs: STADI4 (Stoe & Cie, 1996), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2001).

Selected geometric parameters (Å, º) top
C1—Pt12.036 (10)C4—O11.259 (12)
C2—Pt12.041 (11)N1—Pt12.161 (7)
C3—Pt12.032 (9)N2—Pt12.152 (7)
C4—O21.258 (13)O1—Pt12.168 (6)
O2—C4—O1126.2 (9)C1—Pt1—N1176.5 (4)
C1—Pt1—C285.1 (5)C2—Pt1—N198.2 (4)
C1—Pt1—N299.9 (4)N2—Pt1—N176.7 (3)
C2—Pt1—N2174.8 (5)C3—Pt1—O1176.2 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H22···O10.88 (11)1.96 (11)2.836 (12)172 (15)
O3—H21···O2i0.85 (9)1.96 (10)2.810 (14)177 (11)
Symmetry code: (i) x, y+3/2, z+1/2.
 

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